Optical waveguide and process for manufacturing the same

ABSTRACT

The present invention provides an optical waveguide, which at least includes: a waveguide core having a cavity therein; and a clad which encloses the periphery of the waveguide core and has a smaller refractive index than the waveguide core, wherein the optical waveguide changes a direction of a part or all of propagated light by using a part or all of an interface between the waveguide core and the cavity as a reflecting surface. The present invention further provides a method for manufacturing the optical waveguide, which at least includes: forming a core having a cavity therein on a substrate; applying an uncured clad material to a side surface and an upper portion of the core while maintaining the cavity which allows an atmospheric gas to be present in the cavity; and curing the clad material by heat or light to seal the gas in the cavity.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims priority under 35USC 119 from Japanese PatentApplication No. 2005-162705, the disclosure of which is incorporated byreference herein.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an optical waveguide having thefunction of changing the direction of light propagation.

2. Description of the Related Art

Since the technology of high-speed transmission of signals usingelectricity is approaching its limit, there are great expectations inthe role of optical transmission. In this situation, the realization ofan opto-electric hybrid board is regarded as a today's urgent task. Inorder to realize the opto-electric hybrid board, an optical waveguidecorresponding to a highly integrated electrical device is required. Itis required for the optical waveguide to attain a large change in thedirection of light propagation in a small space within limits imposed bythe integration. A polymer waveguide has a higher degree of designfreedom than a waveguide formed of quartz materials. Although methods ofchanging the direction of light propagation using various polymerwaveguides are being considered, there are problems such as thosedescribed in the following (1) to (3) are imposed.

(1) Problem Relating to Utilizing an Arc

Conventionally, an arc was used for a large change in a direction oflight propagation. However, it is not possible to avoid a loss caused byutilization of a radiation mode when an arc is used. In order to reducethis loss, the arc must have a radius of curvature which is larger thana certain value, giving rise to the necessity for securing a largespace.

(2) Problem Relating to Utilizing a Total Reflection

The use of total reflection by means of a clad is well known. However,since the difference in refractive index between a core and a clad issmall, a large change in direction was not possible. Also, completetotal reflection cannot be performed and there is a leakage of light atthe total reflecting surface.

(3) Problem Relating to Involving the Production of a Mirror Surface bya Dicing Saw

It has been known widely that an optical waveguide is cut at a 45° angleby using a dicing saw and the cut surface is used as a reflecting mirrorto change the direction of a light path. However, it is impossible tocarry out cutting locally. Also, because the polymer optical waveguideis actually cut in this cutting process, it is difficult to attain thiscutting at a place except for the end surface of the optical waveguide.Also, because accuracy of the dicing position is required, leading to anincrease in the number of steps as well bringing about high costs.

Among the aforementioned methods, a method involving measures forsolving the above problems is proposed in which an arc is utilized and aclad is provided within a core (for example, Japanese Patent ApplicationLaid-Open (JP-A) No. 9-145943). In this method, a sandbank-clad isinserted in the arcing layer and the optical waveguide of the bent partis divided into plural narrow-width optical waveguides to greatly reducethe leakage of light. By this method, the reduction in leakage of lightreduces the optical loss and the curvature radius can be made small;however, a limitation to miniaturization remains as before.

As a method of significantly changing the direction of light propagationin a small area, a method can be considered which involves expanding theconditions of total reflection by a localized use of a cladding materialhaving a large difference in refractive index from the core. As anexample of such a method, an air clad is proposed (for example, JP-A No.2003-207661). In this method, an air clad reflecting layer is providedon the exterior of a core in addition to a 90° refraction layer andlight is reflected on the air clad. However, in this method, since theair clad layer is located on the exterior, the manufacturing process iscomplicated and the air clad cannot be easily produced.

Besides the above examples using an air clad, optical waveguides inwhich a closed void (air foam cell) is provided on the exterior of abent part of an optical waveguide core which use the planar interfacebetween the void and the core as a reflecting surface are proposed (forexample, JP-A Nos. 11-248951 and 2003-75670). In all of these opticalwaveguides, voids are also present outside of the core of the opticalwaveguide and the difference in reflection ratios between the void andthe core is utilized to constitute a reflecting surface. In theconfiguration disclosed in JP-A No. 2003-75670, the air clad is formedby etching, but the surface formed by etching tends to be rough, givingrise to the problem that the reflecting surface has a degradedreflecting efficiency. Further, the equipment cost for etching tends tobe higher, and the etching process itself is disadvantageous timewise.Also, because the void is an air cell, the whole end surface of thewaveguide is not completely in contact with the void due to the methodof depositing clad materials and the planar interface is not a perfectlyflat surface, optical loss caused by these reasons is inevitable.

Also, the configurations in JP-A Nos. 11-248951 and 2003-75670 must havethe whole core of the optical waveguide as a total reflecting surface,and it is therefore impossible to make a branched waveguide structure.

Also, in widely used methods in which a Y-branch or the like is used ina branched waveguide to divide light into plural branches, an increasein a branched angle is accompanied by an increase in light leakage andit is therefore impossible to branch light at a wide angle.

The fundamental cause of these problems is a limitation in therefractive indices of the core and the clad to be used because the NAbecomes defined under the conditions of connections between the opticalparts such as a fiber and the like and the optical waveguide.Accordingly, it is conceivable that if a clad, which has a differentrefractive index from that of the core, can be used locally at a placewhere a direction of light propagation is significantly changed, a largechange in the direction of propagation can be realized.

Also, when a polymer having a degree of freedom is used in designing awaveguide, the refractive index of the polymer used for the clad islimited. Therefore, when designing a waveguide without considering NA,such as in the case of directly connecting the waveguide with an opticaltransmitting and receiving device, the clad is not allowed to have arefractive index significantly different from that of the core, with theresult that the direction of light propagation cannot be significantlychanged.

SUMMARY OF THE INVENTION

The present invention provides an optical waveguide having the functionof significantly changing the direction of light propagation by the useof a reflecting surface comprised of an air clad within the opticalwaveguide core, and by taking a large refractive index between the localcore and the clad. The present invention also provides a process formanufacturing the optical waveguide at a low cost with ease.

Namely, the present invention provides an optical waveguide comprising:a waveguide core having a cavity therein; and a clad which encloses theperiphery of the waveguide core and has a smaller refractive index thanthe waveguide core has, wherein the optical waveguide changes adirection of a part or all of propagated light by using a part or all ofan interface between the waveguide core and the cavity as a reflectingsurface.

In one aspect of the optical waveguide of the invention, the cladcomprises a polymer material.

In another aspect of the optical waveguide of the invention, an angle ofthe reflecting surface is set at an inclined angle at which thepropagated light is totally reflected.

In another aspect of the optical waveguide of the invention, an area, inwhich a projected area that is obtained by projecting the reflectingsurface in the direction of the waveguide core overlaps with across-sectional plane of the waveguide core, is smaller than across-sectional area of the waveguide core; and a branched waveguide isformed therein which divides the propagated light incident to thewaveguide core into light which reflects on the reflecting surface andlight, other than light reflected at the reflection surface, whichtravels in linear propagation in the waveguide core.

In another aspect of the optical waveguide of the invention, a branchedwaveguide core that propagates the propagated light reflected on thereflecting surface is provided, and a sectional area of the propagatedlight reflected on the reflecting surface, which is perpendicular to thedirection in which the propagated light travels and is in the vicinityof the branched part, is smaller than the sectional area of the branchedwaveguide core and is contained within the branched waveguide.

In another aspect of the optical waveguide of the invention, an area, inwhich a projected area that is obtained by projecting the reflectingsurface in the direction of the waveguide core overlaps with across-sectional plane of the waveguide core, is identical to across-sectional area of the waveguide core; and the waveguide core isset so as to be larger only at a portion where the cavity is present.

In another aspect of the optical waveguide of the invention, at leastone of both end portions on a diagonal face of the reflecting surface ispositioned outside of a line extending from an outside periphery of thewaveguide core at the upstream side in the direction in which thepropagated light travels, and the waveguide core at the cavity portionis enlarged so as to surround the cavity.

The present invention further provides a method for manufacturing anoptical waveguide, comprising: forming a core having a cavity therein ona substrate; applying an uncured clad material to a side surface and anupper portion of the core while maintaining the cavity which allows anatmospheric gas to be present in the cavity; and curing the cladmaterial by heat or light to seal the gas in the cavity.

In one aspect of the method of the invention, the forming of the corecomprises: preparing a mold which is formed from a curable resin layerof a mold-forming curable resin and has a concave portion correspondingto the convex portion of the waveguide core and a convex portioncorresponding to the cavity; bringing the substrate into close contactwith the mold; filling a core-forming curable resin in the concaveportion of the mold which is in close contact with the substrate; curingthe core-forming curable resin by heat or light; and removing the moldfrom the substrate so as to form a core having a cavity in the interiortherein on the substrate.

The present invention can use the planar interface between the opticalwaveguide core and the cavity as a reflecting surface by providing acavity having a fixed reflecting angle and a fixed reflecting widthwithin the optical waveguide core. The reflection of propagated light ina reduced space can be realized (a large change in the direction oflight propagation can be realized).

Also, if air is selected as the atmospheric gas used after the opticalwaveguide core is produced, a large difference in the refractive indexbetween the core and the air clad can be attained at low cost withoutrequiring special apparatuses.

If the diameter of the waveguide after branching is made larger than thearea of the section perpendicular to the optical axis of reflected lightin the vicinity of the branched part, the reflected light can bepropagated without actually touching an end portion of the branchedpart. It is for this reason that, unlike a conventional Y-branch, theradiation mode loss at the end of the branched part is reduced with theresult that a branched waveguide having reduced excess loss at thebranched part and ability to change the direction of light propagationcan be attained.

An optional branch ratio can be realized by optionally designing thevalid sectional area of the reflecting surface with respect to thepropagation sectional area of the core.

It is difficult to make the end of the reflecting part of the waveguidecore with high precision. There are two end surfaces with respect topropagated light. On the end surface, there are cases where reflectiondos not occur as designed, the direction of reflection differs or lightpasses through the end surface. Consequently, by dispersing the endsurface outside the waveguide core with respect to the propagated light,reflection efficiency is raised and excess loss can be suppressed and achange in the direction of propagation can be realized with reducedloss.

If a reflecting gas clad layer having an area smaller than the area ofthe section of the waveguide whose section is perpendicular to thedirection of light propagation is proposed, propagated light can bepartially reflected and a wide-angle branched waveguide can be realized.

The present invention does not have a 45° cutting step or the like usinga dicing saw or the like to realize a change in the direction of lightpropagation and is therefore simple and inexpensive.

The manufacturing process of the present invention is simple and lowcost. Also, because a mold is used, reproduction becomes possible,making it possible to realize the manufacturing at lower cost.

From the above, the direction of propagated light can be significantlychanged locally by the present invention, and a flexible opticalintegrated circuit, which could not be attained conventionally, can nowbe produced.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic view showing a typical example of a waveguide coreof an optical waveguide to which the present invention has been applied;

FIG. 2 are explanatory diagrams view showing different states of thewaveguide core of the optical waveguide shown in FIG. 1;

FIG. 3 is a view corresponding to FIG. 1 which explains a validreflection area in the optical waveguide;

FIG. 4 is a view showing an extreme example of a configuration of theoptical waveguide shown in FIG. 3;

FIG. 5 are conceptional views showing an embodiment of the steps ofmanufacturing the optical waveguide of the present invention;

FIG. 6 is a perspective view showing a situation in which a mold isbrought into close contact with a substrate for a clad;

FIG. 7 is a view corresponding to FIG. 1 which shows the opticalwaveguide of Example 1;

FIG. 8 is a view corresponding to FIG. 1 which shows the opticalwaveguide of Example 2; and

FIG. 9 are views corresponding to FIG. 1 which shows the opticalwaveguide of Example 3.

DETAILED DESCRIPTION OF THE INVENTION

Optical Waveguide

The optical waveguide of the invention is characterized by having atleast a waveguide core having a cavity therein and a clad which enclosesthe periphery of the waveguide core and has a smaller refractive indexthan the waveguide core. The optical waveguide changes a direction of apart or all of propagated light by using a part or all of an interfacebetween the waveguide core and the cavity as a reflecting surface.

An embodiment of the optical waveguide of the present invention will beexplained with reference to FIG. 1. FIG. 1 is a schematic view showingonly a waveguide 70 in an example of an optical waveguide to which thepresent invention is applied. The waveguide core 70 is constituted of amain waveguide core 72 and a branched waveguide core 74, and a cavity 76is positioned at the branched part between the main waveguide core 72and the branched waveguide core 74. The cavity 76 has a right-angle anda slanted surface facing the right-angle and the slanted surface forms areflecting surface due to a difference in the refractive index betweenthe waveguide core 70 and the cavity 76. That, is, among the propagatedlight incident from an incident side 1 of the waveguide core 70,propagated light that is not affected by the cavity 76 but travelsstraight is emitted from an emitting side 2 whereas propagated lightreaching the cavity 76 is reflected on the reflecting surface of thecavity 76 in the core and emitted from a reflecting side 3.

Specifically, the optical waveguide of the present invention has acavity having a reflecting angle and an amount of reflected light thatare optically set inside of the waveguide core to make use of the planarinterface between the cavity and the waveguide core to realize a changein the direction of light propagation by utilizing a relatively largedifference in refractive index between the core and the medium insidethe cavity. The cavity is regarded substantially as a local gas cladinside of the waveguide core. When, for example, the optical waveguidecore has a refractive index of 1.5 and the medium in the cavity is air,total reflection can be realized at an angle up to 41.8° with referenceto the normal of the reflecting surface (93.2° to the direction ofpropagation).

More specifically, when the following conditions are selected to designthe waveguide core made of a polymer: refractive index of the core:1.55, gas in the cavity: air, and the critical angle with the directionof the normal of the reflecting surface: approximately 40°. When theangle of the reflecting surface with respect to the direction of lightpropagation is 45°, total reflection is possible and as a result, achange in the direction of light propagation of an angle 90° can beattained.

Namely, the above reflecting surface may be designed to have a slantedangle at which the propagated light is totally reflected. When therefractive index of the waveguide core is n_(c) and the refractive indexof the medium in the cavity is n_(g), the critical angle for totalreflection is given by:θ=sin⁻¹(n _(g) /n _(c))

Also, when an optical fiber is connected to the incident side 1 oremitting side 2 of the optical waveguide or to the reflecting side 3, adifference in NA is pointed out from the viewpoint of connection loss oflight. However, in this embodiment, an NA constituted of the refractiveindex of the core of the optical waveguide and the clad whollysurrounding the core is applied, and does not contribute to therefractive index of the cavity in the waveguide core.

Also, if the reflecting surface of FIG. 1 takes the same angle as or anangle very close to the total reflecting angle, the propagated light canbe divided into totally reflected light and partially transmitted lightwith the result that a branched waveguide can be realized.

Also, the waveguide can be formed as a branched waveguide in which thearea where the projected area when the above reflecting surface isprojected in the direction of the waveguide core overlaps with thesectional area of the waveguide core is smaller than the sectional areaof the waveguide core and the propagated light incident to the waveguidecore is divided as branches into light reflecting on the reflectingsurface and light that propagates within the waveguide core except atthe above reflecting surface and travels linearly. In other words, whenthe light incident to the reflecting surface is smaller than thereflecting surface side core diameter as viewed from the incident side,it is changed in its direction of propagation by reflection and thelight which is not incident to the reflecting surface is not changed inits direction and propagates as it is in the main waveguide, and, as aresult, a wide-angle branched waveguide can be realized.

Also, when the area (valid reflection area) where the projected areawhen the above reflecting surface is projected in the direction of thewaveguide core overlaps with the sectional area of the waveguide core isthe same as the sectional area of the waveguide core, or, in otherwords, when the size of the effective reflecting surface is the same asthe core diameter as viewed from the incident side, the direction ofpropagation of propagated light of the main waveguide is changed bytotal reflection on the reflecting surface.

Here, the valid reflection area will be explained. Here, the directionof light propagation approximates to a parallel direction with respectto the core. FIG. 3 is a view for explaining the valid reflection areawherein the same elements as in FIG. 1 are represented by the samesymbols. In FIG. 3, arrow A shows the sectional area of the waveguidecore (main waveguide 72), arrow C shows the projected area in the caseof projecting at the reflecting surface in the direction of thewaveguide core and arrow B shows the area where arrow A and arrow Coverlaps each other, and this overlapping area is the valid reflectionarea. Hereinafter, the part corresponding to the valid reflection areainside of the waveguide core is referred to as a valid core part.

In the branched waveguide 74, on the other hand, arrow D shows thesectional area of the branched waveguide 74, arrow E shows the area,namely, the valid reflection area where the area of the section of thepropagated light is reflected on the reflecting surface, which is asection perpendicular to the direction of travel of the propagated lightin the vicinity of the branched part that overlaps on the branchedwaveguide plane, and arrow F shows the projected area when thereflecting surface is projected in the direction of the branchedwaveguide.

Also, the optical waveguide of the present invention is preferablyprovided with a branched waveguide core that propagates the propagatedlight reflected on the reflecting surface, and this area (arrow E inFIG. 3) where the area of the section of the propagated light isreflected on the reflecting surface, which is a section perpendicular tothe direction of travel of the propagated light in the vicinity of thebranched part hat overlaps with the branched waveguide plane, ispreferably smaller than the sectional area (arrow D in FIG. 3) of thebranched waveguide core and is preferably included in the branchedwaveguide. If the optical waveguide is designed as above, the opticalloss at the branched end portion can be reduced.

It is to be noted that the optical waveguide of the present inventionmay have a configuration in which the area of the section of thepropagated light reflected on the reflecting surface, which is a sectionperpendicular to the direction of travel of the propagated light in thevicinity of the branched part is not included in the branched waveguide.This configuration will be explained with reference to FIG. 4. In FIG.4, the same elements as in FIG. 1 or FIG. 2 are represented by the samesymbols. In FIG. 4, arrow A shows the sectional area of the waveguidecore (main waveguide 72), arrow B shows the projected area in the caseof projecting light at the reflecting surface in the direction of thewaveguide core, and arrow C shows the area where arrow A and arrow Boverlap each other and is, specifically, the valid reflection area. Inbranched waveguide 74, similarly, arrow D shows the sectional area ofbranched waveguide 74, arrow E shows the area, namely, the validreflection area where the area of the section of the propagated light isreflected on the reflecting surface, which is a section perpendicular tothe direction of travel of the propagated light in the vicinity of thebranched part that overlaps with the branched waveguide plane, arrow Fis the area of the section of the reflected propagated light, which is asection perpendicular to the direction of travel of the propagated lightin the vicinity of the branched part, and arrow G shows the projectedarea when the reflecting surface is projected in the direction of thebranched waveguide. Specifically, in the configuration shown in FIG. 4,the light (arrow F) reflected on the reflecting surface deviates fromthe branched waveguide 74.

Also, both end portions of the reflecting surface side of the cavity aresometimes rounded or made at an angle different from the intendedreflecting angle. Thereby, the angle of a change in the direction oflight propagation is made different from the intended one, resulting inlight leakage to the clad, leading to the loss of propagated light. Toprevent this, the end of the reflecting surface of the gas cavity ispositioned on the outer side on the outside of valid core part of thepropagated light of the main waveguide, thereby avoiding the adverseinfluence of the ends of the reflecting surface (see FIG. 2A to FIG.2C). In the branched waveguide, either one of the ends of the reflectingsurface can be positioned outside of the valid core part of the mainwaveguide (FIG. 2A and FIG. 2B). Here, the configuration of FIG. 2B isbetter because the effect of angle expansion of the reflected light inthe main waveguide is reduced. Also, in the case of changing thedirection of all the propagated light, it is required only for thereflecting surface to have a larger area than the valid sectional areaof the main waveguide. In this case, it is therefore only required forboth of the reflecting surfaces to be positioned outside of the validsectional area of the main waveguide core (FIG. 2C). Either one or bothend portions in a diagonal face of the reflecting surface is/arepositioned outside of the line extended from the outside of thewaveguide core at the upstream side in the direction of travel of thepropagated light, and the waveguide core at the cavity part is enlargedin such a manner as to surround the cavity.

As mentioned above, the optical waveguide of the present inventionchanges the direction of light propagation by using the interfacebetween the waveguide core and the cavity as a reflecting surface. Thissystem has the advantage that it makes it possible to change thedirection of light propagation locally in a reduced space and also toform a good reflecting surface since the reflecting surface made of agas cavity is positioned adjacent to the waveguide core in the waveguidecore.

The aforementioned optical waveguides of the present invention arepreferably used in multi-mode.

Next, explanations will be furnished as to the process for manufacturingan optical waveguide of the present invention, the process being able tomanufacture the optical waveguide of the present invention.

The process for manufacturing an optical waveguide of the presentinvention at least includes: (1) forming a core having a cavity thereinon a substrate; (2) applying an uncured clad material to a side surfaceand an upper portion of the core while maintaining the cavity whichallows an atmospheric gas to be present in the cavity; and (3) curingthe clad material by heat or light to seal the gas in the cavity.

Hereinafter, the process for manufacturing an optical waveguideaccording to the present invention will be explained in the order.

(1) Formation of a Core Having a Cavity therein on a Substrate

The formation of a core having a cavity therein particularly preferablyinvolves the following a) to e):

(a) preparing a mold which is formed from a curable resin layer of amold-forming curable resin and has a concave portion corresponding tothe convex portion of the waveguide core and a convex portioncorresponding to the cavity;

(b) bringing the substrate into close contact with the mold;

(c) filling a core-forming curable resin in the concave portion of themold which is in close contact with the substrate;

(d) curing the core-forming curable resin by heat or light; and

(e) removing the mold from the substrate so as to form a core having acavity in the interior therein on the substrate.

According to the method for manufacturing an optical waveguide accordingto the present invention, the optical waveguide of the present inventioncan be produced simply because in the formation of the cavity, it isunnecessary to carry out other steps such as an etching step and it isalso unnecessary to install any apparatus for carrying out these othersteps and the cavity is formed simultaneously when the waveguide core isformed. Also, in the process for manufacturing an optical waveguideaccording to the present invention, the plane which is to be thereflecting surface in the cavity depends on a precision of the planecorresponding to the cavity in the mold, therefore the precision of thereflecting surface can be easily improved by improving the precision ofthe plane of the mold.

Hereinafter, a preferable embodiment of the formation (1), specificallythe aforementioned (a) to (e) will be hereinafter explained.

(a) Preparation of a Mold which is Formed from a Curable Resin Layer ofa Mold-Forming Curable Resin and has a Concave Portion Corresponding tothe Convex Portion of the Waveguide Core and a Convex PortionCorresponding to the Cavity

The mold is preferably produced using a master plate provided with aconvex portion corresponding to the optical waveguide core and a concaveportion corresponding to the cavity though the method of producing themold is not limited thereto. This method using the master plate will beexplained.

Production of a Master Plate

A conventional method, such as a photolithographic method, may be usedwithout any particular limitation to produce the master plate providedwith a convex portion corresponding to the optical waveguide core and aconcave portion corresponding to the cavity. The polymer opticalwaveguide manufacturing method using an electrodeposition method or aphotoelectric deposition method, that is previously filed by theapplicant of this case as the patent application Japanese PatentApplication No. 2002-10240, may also be used to produce the masterplate. A size of the convex portion corresponding to the opticalwaveguide core is properly decided according to, for example, an objectof a utilization of the polymer waveguide. For example, when the opticalwaveguide is intended for a single mode one, a core which is an about 10μm by 10 μm square is usually used. when the optical waveguide isintended for a multi-mode optical waveguide, a core which is an about 50to 100 μm by 50 to 100 μm square is usually used. An optical waveguidehaving a larger core part having a size of several hundreds of μm mayalso be utilized in accordance with an intended use thereof.

Production of a Mold

A mold-forming curable resin is applied to or cast into a surface of themaster plate produced as mentioned above on which the convex portioncorresponding to the optical waveguide core and the concave portioncorresponding to the cavity are formed. The resin is then allowed tostand for a certain period and subjected to a defoaming operation undervacuum for about 10 minutes. After the thus obtained resin layer isdried in accordance with necessity, this resin is cured, and then thecured resin layer is removed so as to form the mold. The mold is formedso as to have an introduction port for filling the concave portioncorresponding to the above convex portion with a core-forming curableresin and a discharging port for discharging the resin from the concaveportion corresponding to the convex portion. There is no particularlimitation to a method for forming the ports. Convex portionscorresponding to the introduction port and discharge port may be formedon the master plate in advance. A method is also given as an example ofa simple method therefor, in which both ends of the mold that has beenremoved from the master plate as described above are cut such that theabove convex portions are exposed to form an introduction port and adischarge port.

An appropriate thickness of the curable resin layer is generally in arange of about 0.1 to 50 mm, though it is properly determined intoconsideration of handling characteristics required thereto as a mold.

Also, it is desirable to promote removing of the mold from the masterplate by subjecting the master plate to a releasing treatment such as anapplication of a releasing agent in advance.

The mold-forming curable resin preferably has properties that: a curedmaterial thereof is easily removed from the master plate; a mechanicalstrength and a dimensional stability thereof are certain levels or moreso as to be suitable as a mold that is repeatedly used; having ahardness that is enough to maintain the shapes of the concave portionand the convex portion; and having excellent adhesiveness so as toclosely contact to the cladding substrate. Various kinds of additivesmay be added to the mold-forming curable resin as needs arise.

The mold-forming curable resin is necessary being capable of coated orinjected on a surface of the master plate and being capable ofaccurately copying the convex portions corresponding to respectiveoptical waveguide cores and the convex portions corresponding to therespective cavities. Accordingly, the mold-forming curable resinpreferably has a viscosity equal to or less than a certain limit, forinstance, approximately from 500 to 7000 mPa·s. (The “mold-formingcurable resin” used in the invention includes ones that become anelastic rubber-like body after curing in its scope.) Further, a solventfor adjusting the viscosity may be added to an extent that does notexhibit adverse affect of the solvent.

Examples of the mold-forming curable resin which are preferable fromviewpoints of removability, mechanical strength, dimensional stability,hardness, and adhesiveness with the cladding substrate as mentionedabove include curable organo-polysiloxanes that become a silicone rubber(silicone elastomer) or a silicone resin after curing. Preferableexamples of the curable organo-polysiloxane include those having amethyl siloxane group, an ethyl siloxane group or a phenyl siloxanegroup in a molecule thereof. The curable organo-polysiloxane may beeither a one-component type or a two-component type in which a curingagent is combined. Further, the curable organo-polysiloxane may beeither a heat-curable type and a room temperature-curable type (forinstance, one that is cured by moisture in air). Furthermore, thecurable organo-polysiloxane may be one that uses other curing system(such as UV curing or the like).

The curable organo-polysiloxane is preferably one that becomes siliconerubber after curing. Preferable examples thereof include one that isordinarily called a liquid silicone rubber (the “liquid” includes onethat is high in the viscosity such as a pasty one in its scope) which isused in combination with a curing agent for a two-component type resin.Among these, an addition type liquid silicone rubber is preferably usedsince it can be uniformly cured from surface to the inside thereof in ashort period of time, generates no or little by-product during curing,is excellent in a mold-releasing property and has small shrinkage rate.

Among the liquid silicone rubbers, a liquid dimethyl siloxane rubber isparticularly preferable from the viewpoints of adhesiveness,removability, strength and hardness.

A viscosity of the liquid silicone rubber is preferably in a range ofapproximately from 500 to 7,000 mPa·s, and more preferably in a range ofapproximately from 2,000 to 5,000 mPa·s, from the viewpoints of accuratecopying of the convex portions corresponding to the optical waveguidecores and the concave portions corresponding to the cavities, reducingair bubbles mingle and thereby making vaccum defoaming easier, andforming the mold having a thickness of several millimeters.

Further, a surface energy of the mold is in a range of approximately 10to 30 dyn/cm, and preferably in a range of approximately 15 to 24dyn/cm, in view of adhesiveness thereof with the substrate.

A Share rubber hardness of the mold is in a range of approximately 15 to80 and preferably in a range of approximately 20 to 60 from theviewpoints of a molding performance, maintenance of shape of the concaveportion and the removability thereof.

A surface roughness (root-mean-square (RMS) roughness) of the mold isapproximately 0.2 μm or less and preferably approximately 0.1 μm or lessfrom the viewpoint of the molding performance thereof.

Further, the mold is preferably transmissive for light which is in UVregion and/or visible region. The reason for the mold being preferableto be light transmissive in the visible region is that when the mold isbrought into close contact with the cladding substrate in the process(2) described below, positional alignment can be easily performed, andin the process (3) described below, the situations where the coreforming curable resin is filled in the mold concave portion can beobserved and thereby completion of the filling and the like can beeasily confirmed. Further, the reason for the mold being preferable tobe light transmissive in the UV region is that in the case of a UVcurable resin being used as the core forming curable resin, the UV lightcuring is performed through the mold. In this case, the transmittance ofthe mold in the UV region (from 250 to 400 nm) is preferablyapproximately 80% or more.

The curable organo-polysiloxane, particularly the liquid silicone rubberthat becomes silicone rubber after being cured, is excellent in theproperties of adhesiveness with the cladding substrate and removabilitytherefrom, which are usually incompatible with each other. It has thecapability of copying a nanostructure, and can also prevent an intrusionof liquid when the silicone rubber and the cladding substrate arebrought into close contact. The mold that uses such silicone rubber cancopy an master plate with high precision and come into close contactwith the cladding substrate, therefore, an interface between the coreand the cavity, that is the reflecting surface, and an interface betweenthe core and the clad around the core, that is a side surface of thecore, are formed in extremely good condition. Further, the core formingresin can be efficiently filled only in the concave portion between themold and the cladding substrate, and the cladding substrate and the moldcan be easily removed. Accordingly, a polymer optical waveguide thatmaintains a shape with high precision can be extremely easily preparedby using the mold.

Further, a portion of the cured resin layer which is other than aportion that copies a convex portion and the concave portion of themaster plate can be replaced by other stiff material so as to improve ahandling property of the mold. The improvement effect is remarkable inthe case that the cured resin layer has a rubber elasticity.

(b) Bringing the Substrate into Close Contact with the Mold

A material of the substrate of the optical waveguide of the invention isselected in consideration of optical characteristics such as arefractive index, light transmittance or the like, mechanical strength,heat-resistance, flexibility and the like of the material in accordancewith the applications thereof. It is preferable to prepare a polymeroptical waveguide having the flexibility by using a flexible filmsubstrate.

Examples of a material of the film include acrylic resins (such aspolymethyl methacrylate or the like), alicyclic acrylic resins, styrenicresins (such as polystyrene, acrylonitrile/styrene copolymer or thelike), olefinic resins (such as polyethylene, polypropylene,ethylene/propylene copolymer or the like), alicyclic olefinic resins,vinyl chloride resins, vinylidene chloride resins, vinyl alcohol resins,vinyl butyral resins, allylate resins, fluorine-containing resins,polyester resins (such as polyethylene terephthalate, polyethylenenaphthalate or the like), polycarbonate resins, di- or triacetatecelluloses, amide resins (such as aliphatic amides, aromatic amides orthe like), imide resins, sulfonic resins, polyether sulfonic resins,polyether ether ketone resins, polyphenylene sulfide resins,polyoxymethylene resins, or compsitions formed by blending the aboveresins.

Examples of the alicyclic acrylic resin include OZ-1000, OZ-1100 (bothtrade names, manufactured by Hitachi Chemical Co., Ltd.) in that analiphatic cyclic hydrocarbon such as tricyclodecane or the like isintroduced in an ester substituent.

Further, examples of the alicyclic olefinic resin include those having anorbornene structure on a main chain and those having a norbornenestructure on a main chain and a polar group such as an alkyloxycarbonylgroup (alkyl group with from 1 to 6 carbon atoms or cycloalkyl group) ona side chain. Among these, alicyclic olefinic resins as mentioned abovethat have a norbornene structure on a main chain and a polar group suchas an alkyloxycarbonyl group on a side chain have excellent opticalcharacteristics such as low refractive index (since the refractive indexis approximately 1.50, the difference with the refractive index of thecore clad can be secured) and high light transmittance, excellentadhesiveness with the mold, and excellent heat-resistance. Accordingly,these are particularly preferable for the preparation of a polymeroptical waveguide according to the invention.

In view of securing the refractive index difference with the core, therefractive index of the substrate is preferably less than approximately1.55, and more preferably less than approximately 1.53.

Further, a substrate in which a clad material is coated thereon can alsobe used as the cladding substrate. A utilization of such substrate canimprove a flatness of the substrate of the optical waveguide of thepresent invention. Furthermore, a material that has high birefringenceand is not suitable for the clad material, or a material that isinferior in transparency, also can be made usable as the substrate ofthe optical waveguide of the present invention when it is coated withthe clad material as described above.

(c) Filling a Core-Forming Curable Resin in the Concave Portion of theMold which is in Close Contact with the Substrate

In the filling process, a core forming curable resin is filled in aconcave portion of a mold other than a convex portion of the moldcorresponding to the cavity from the inlet of the mold by utilizing acapillary phenomenon, while the core forming curable resin filled in theconcave portion is exhausted from the outlet of the mold.

Examples of the core forming curable resin include radiation curableresins, electron beam curable resins, and thermosetting resins. Amongthese, UV curable resins and thermosetting resins can be preferablyused.

Examples of the core forming UV curable resins or thermosetting resinsinclude UV curable monomers, thermosetting monomers, UV curableoligomers, thermosetting oligomers, mixtures of UV curable monomer andUV curable oligomer, and mixtures of thermosetting monomer andthermosetting oligomer.

Examples of the UV curable resin include UV curable epoxy resins, UVcurable polyimide resins, and UV curable acrylic resins.

In order to fill a gap (concave portion of the mold) formed between themold and the substrate with a core forming curable resin by capillaryphenomenon, the core forming curable resin that is used necessarily hasa low viscosity that is enough to enable such filling process.Accordingly, the viscosity of the curable resin is adjusted in a rangeof approximately 10 to 2,000 mPa·s, preferably from approximately 20 to1,000 mPa·s, and more preferably from approximately 30 to 500 mPa·s.

In addition, in order to reproduce original shapes, which the convexportion corresponding to the optical waveguide core and the concaveportion corresponding to the cavity formed on the master plate has, withhigh fidelity, a volume change (difference) between a volume of beforethe curing and a volume of after the curing of the curable resin isnecessarily small. For instance, a decrease in the volume of the curableresin causes a loss of the waveguide. Accordingly, the volume change ofthe curable resin is desirably as small as possible; that is, it isdesirable to be approximately 10% or less and preferably approximately6% or less. A lowering of the viscosity by use of a solvent is desirablyavoided since such an adjustment causes a large volume change between avolume of before the curing and a volume of after the curing.

In order to reduce the volume change (shrinkage) after the curing of thecore forming curable resin, a polymer can be added to the resin. As thepolymer, one that is compatible with the core forming curable resin anddoes not adversely affect on the refractive index, elasticity and lighttransmittance of the resin is preferable. The addition of the polymerenables to precisely control the viscosity and the glass transitiontemperature of the cured resin, in addition to redicing the volumechange. Examples of the polymer include acrylic resins, methacrylicresins, and epoxy resins, however, the polymer is not limited thereto.

A refractive index of the cured body of the core forming curable resinis necessarily larger than that of the substrate to be a clad (includingthe cladding layer in the following (d)). The refractive index should beapproximately 1.50 or more, and preferably approximately 1.53 or more.The difference between the refractive index of the clad (including thecladding layer in the following (d)) and that of the core is greater0.01 or more and preferably greater 0.03 or more.

Further, in order to promote the filling of the core forming curableresin into the mold concave portion by capillary phenomenon, a totalsystem of the process is preferably set in a reduced pressure(approximately from 0.1 to 200 Pa) or suctioned by use of a throughcavity.

Furthermore, in order to expedite the filling, in addition to thereduction of pressure of the system, the core forming curable resin thatis filled in from the inlet of the mold can be effectively heated tolower the viscosity.

(d) Curing the Core-Forming Curable Resin by Heat or Light

The filled core forming curable resin is cured. In curing a UV curableresin, a UV lamp, UV LED, UV irradiation device and so on are used.Furthermore, in curing a thermosetting resin, an oven or the like isused for heating.

(e) Removing the Mold from the Substrate so as to Form a Core Having aCavity in the Interior therein on the Substrate

After the process (d), the mold is removed from the substrate.

A core having a cavity therein is formed by the above steps. However, amethod of producing a core having a cavity therein on a substrate is notlimited to the above production method and, for example, a directexposure method and an etching method may be applied. However, the abovemethod is preferably selected from the viewpoint of cost and simplicity.

(2) Applying an Uncured Clad Material to a Side Surface and an UpperPortion of the Core While Maintaining the Cavity which Allows anAtmospheric Gas to be Present in the Cavity

In this application, a clad layer is formed on the film substrate, whichis obtained by above forming process of (1) and formed with the core. Asto the technologies for applying an uncured clad material to the sidesurface and the upper part of the core while keeping the above cavity,it is preferable to use a highly viscous curable resin as the cladmaterial. Specifically, the gas is confined within the cavity in thecore by applying a non-solid clad (uncured clad material) to the sidesurface and upper part of the core. A highly viscous curable resin ispreferably used to stop the amount of the clad material entering thecavity. A viscosity of the resin is preferably in a range ofapproximately 30 mPa·s to 3000 mPa·s from the viewpoint of compatibilitywith productivity, and more preferably in a range of approximately 100mPa·s to 2000 mPa·s from the viewpoint of yield.

As the clad curable resin, an ultraviolet-curable resin or aheat-curable resin is preferably used. For example, anultraviolet-curable or heat-curable monomer or oligomer and a mixture ofa monomer and an oligomer is used.

In order to reduce a reduction in volume (shrinkage) after theclad-forming curable resin is cured, a polymer (e.g., a methacrylic acidtype and epoxy type) that has compatibility with the resin and noadverse influence on the refractive index, elastic modulus andtransmission characteristics of the resin may be added to the resin.

Here, because the atmosphere in this step constitutes a medium in thecavity as it is, this step is carried out in the atmosphere of the gas,which is intended to be present inside of the cavity. As the gas, air ispreferable because it is simplest and also from the viewpoint of cost.

Polymers which are similar to the polymer to be added to the clad layermay be added thereto so as to reduce a change (shrinkage) in a volume ofthe ultraviolet curable resin or heat-curable resin after the resin iscured.

The refractive index of the clad layer is approximately 1.55 or less andpreferably approximately 1.53 or less to secure the difference inrefractive index between the clad layer and the core. Also, a differencein refractive index between the substrate for the clad and the cladlayer is preferably small and the difference is preferably approximately0.05 or smaller, preferably approximately 0.001 or smaller, and morepreferably approximately zero (no difference) from the viewpoint ofconfining light.

In a method of manufacturing an optical waveguide according to theinvention, in particular, a combination where as the mold-formingcurable resin, liquid silicone rubbers that become rubber-like formafter curing, especially liquid dimethyl siloxane rubber, is used and asthe cladding substrate, an alicyclic olefinic resin that has anorbornene structure on a main chain and a polar group such as analkyloxycarbonyl group, etc. on a side chain is used is preferable. Inthis combination, adhesiveness between the mold and the claddingsubstrate is quite good, the concave portion structure of the mold doesnot deform, a curable resin can be speedily filled into the concaveportion owing to the capillary phenomenon even when a cross sectionalarea of the concave portion structure is extremely small (for instance,a rectangle of 10×10 μm).

(3) Curing the Clad Material by Heat or Light to Seal the Gas in theCavity

In this curing, in succession to the applying process (2), the cladmaterial is cured by heat or light to confine the gas in the cavity andalso to complete an optical waveguide.

In curing a UV curable resin as a clad material, a UV lamp, UV LED, UVirradiation device and so on are used. Furthermore, in curing athermosetting resin, an oven or the like is used for heating.

Next, an embodiment of the forming process (1) will be explained withreference to FIG. 5 and FIG. 6. The following explanations show aprocess of producing a non-branched linear optical waveguide wherein acavity is omitted for the sake of explanation simplicity.

FIG. 5A to FIG. 5G are conceptional views showing each production stagein the manufacturing method according to the present invention, and FIG.6 is a perspective view showing the situation (step shown by FIG. 5D)where a mold is brought into close contact with a substrate for a cladwhich is one pitch larger than the mold.

FIG. 5A shows a section of a master plate 10 when the master plate 10formed with a convex portion 12 corresponding to an optical waveguidecore is cut at a right angle with the longitudinal direction of theconvex portion 12.

Then, as shown in FIG. 5B, a cured resin layer 20 a of a mold-formingcurable resin is formed on the surface of the master plate on whichsurface the convex portion 12 is formed. FIG. 5B shows a section of amaster plate 10 when the master plate 10 formed with a cured resin layer20 a of a mold-forming curable resin is formed is cut at a right anglewith the longitudinal direction of the convex portion 12.

Then, the cured resin layer 20 a of a mold-forming curable resin isremoved off to make a model (not shown) and then both ends of the moldare cut such that the above concave portions 22 are exposed to form anintroduction port 22 a (see FIG. 6) for filling a core-forming curableresin in the concave portion 22 and a discharge port 22 b (see FIG. 6)for discharging the above resin from the concave portion 22corresponding to the above convex portion 12, to produce a mold 20.

A substrate 30, that is a substrate for a clad, is brought into closecontact with the mold 20 produced in this manner (see FIG. 5D and FIG.6). FIG. 5D shows a sectional view taken at right angle with alongitudinal direction of the concave portion of the mold with which thesubstrate is into close contact (A-A section in FIG. 6). Next, acore-forming curable resin 40 a is filled in the concave portion 22 ofthe mold from the introduction port 22 a of the mold by utilizing acapillary phenomenon. The core-forming curable resin is discharged fromthe discharge port 22 b disposed at the other end of the concave portion20. FIG. 5E shows a sectional view taken at right angle with thelongitudinal direction of the concave portion of the mold in which acurable resin is filled in the concave portion.

Then, the core-forming curable resin in the concave portion of the moldis cured to remove off the mold. FIG. 5F shows a sectional view taken atright angle with the longitudinal direction of the core of the opticalwaveguide in which the optical waveguide core 40 is formed on thesubstrate for the clad.

Then, in the present invention, the above core is placed under theatmosphere of the gas which is desirably filled in the cavity and a cladmaterial is applied to the surface of the substrate for the clad onwhich surface the core is to be formed and as a result, a clad layer 50is formed without any penetration of the clad agent into the cavitybecause of the viscosity of the clad agent. Then, the clad resin iscured to produce an optical waveguide 60. FIG. 5G shows a sectional viewwhen the polymer optical waveguide 60 is cut at right angle with thelongitudinal direction of the core.

Further, in a method of manufacturing an optical waveguide according tothe invention, it is preferable that the mold is provided with two ormore through cavities that communicate, respectively, with one ends andthe other ends (inlets and outlets for filling or exhausting the coreforming curable resin) of the concave portions corresponding to theoptical waveguide core convex portions; and into the through cavity atone end of the concave portion of the mold, the core forming curableresin is filled in, and from the through cavity at the other end of theconcave portion of the mold, vacuum suction is applied to fill the coreforming curable resin in the concave portion of the mold. By filing thecore forming curable resin by use of the mold as mentioned above, thefilling speed can be drastically increased, adhesiveness between themold and the substrate is further improved and air bubbles can beinhibited from mingling.

Two or more through cavities can be disposed. In the case of there beingfor instance one Y branch, three through cavities are necessary to bedisposed, and in the case of there being three Y branches to form 1 to 8branching, nine through cavities are necessary to be disposed to fillthe core forming curable resin in the concave portions. Furthermore, thebranching can include multi-stage branching.

The through cavity that is disposed on a side of an inlet of the coreforming curable resin has a function of a liquid (core forming curableresin) reservoir. Furthermore, the through cavity that is disposed on aside of an outlet of the core forming curable resin is used, when theresin is filled in the concave portion of the mold, to perform vacuumsuction to reduce pressure of the concave portion of the mold. There areno particular restrictions on a shape and a magnitude of the throughcavity on the inlet side as far as the through cavity communicates withan inlet end of the concave portion and has a function as a liquidreservoir. Further, there are no particular restrictions on a shape anda magnitude of the through cavity on the outlet side as far as thethrough cavity communicates with an outlet end of the concave portionand can be used to apply the vacuum suction.

The through cavity disposed on the side of the inlet of the core formingcurable resin of the mold concave portion has a function as a liquidreservoir. Accordingly, when a sectional area thereof, in the case ofthe mold being brought into close contact with the cladding substrate,is made larger on a side that comes into contact with the substrate andsmaller as departs from the substrate, after the core forming curableresin is filled in the concave portion and cured, the mold becomeseasily removed from the substrate. Since there is no need of providing afunction of a liquid reservoir to the through cavity on the side of theoutlet of the core forming curable resin, there is no need ofparticularly adopting such a sectional structure.

The mold with the through cavities can be formed, for instance, in sucha way that a mold in which concave portions corresponding to opticalwaveguide core convex portions are formed and convex portionscorresponding to the cavities as mentioned above is prepared, the moldis punched out into a predetermined shape to form through cavities, and,at this time the mold is punched out so that, inside of the throughcavities, an inlet for filling the core forming curable resin and anoutlet for exhausting the core forming curable resin from the concaveportion may appear. Even in the case of the punched out throughcavitiesince adhesiveness between the mold and the cladding substrate isexcellent and a gap is not formed with the cladding substrate except forthe mold concave portion, there are no worries of the core formingcurable resin intruding into other than the concave portion.

Furthermore, the through cavity may be formed not only by removing allof the cured resin layer (punched out type) in a thickness direction ofthe mold as mentioned above but also by partially leaving the mold in athickness direction of the mold. In this case, the mold is disposed sothat the through cavity may be exposed below the cladding substrate.

Examples of the preparation of the mold with the through cavitiesfurther include a method in which an master plate is provided with notonly convex portions corresponding to the optical waveguide cores butalso with convex portions for forming the through cavities (in the caseof punched out through cavities, a height of this convex portion is madehigher than a thickness of the cured resin layer of the mold-formingcurable resin); on the master plate the mold-forming curable resin iscoated so that the convex portions for the through cavities may punchthrough the resin layer (punched out through cavity) or the convexportions may hide; subsequently, the resin layer is cured; and,thereafter, the cured resin layer is removed from the master plate.

It is clear that methods of forming a waveguide core are not limited tothe above methods and it is possible to produce a core having a cavitythat constitutes a reflecting surface on a substrate by a directexposure method or an etching method.

Also, in the present invention, the configuration in which the cavity isformed inside the optical waveguide core may be a configuration in whichthe side surfaces of the core are enclosed by the waveguide core and thetop and bottom of the core are sealed by the clad by allowing the cavityto penetrate the waveguide core, a configuration in which only one ofthe top and bottom of the cavity is in contact with a clad or aconfiguration in which the whole periphery of the cavity is enclosed inthe waveguide core. However, the configuration in which the top andbottom of the core are in contact with the clad by allowing the cavityto penetrate the waveguide core is preferable because signal lights thatpropagate in the waveguide core is scarcely scattered at the top andbottom of the cavity.

EXAMPLES

The present invention will be hereinafter explained in more detailillustrated by the following examples, however the present invention isnot limited to these examples.

Example 1

As shown in FIG. 7, a main waveguide is 100 μm by 100 μm and has alength of 20 mm, a gas cavity constituted of air has a configurationwhich is an isosceles triangle structure in which the sides forming aright angle are each 50 μm in length and has a plane inclined at anangle of 45° in the direction of light propagation in the main waveguideand disposed at the center of the main waveguide and a branchedwaveguide which is 100 μm by 100 μm and has a length of 5 mm. Aultraviolet ray-curable polymer having a refractive index of 1.54 isused for a core, a ultraviolet ray-curable polymer having a refractiveindex of 1.51 is used as a clad and ARTON FILM® (manufactured by JSRCorporation) is used as a bottom substrate. An LED having a wavelengthof 850 nm is disposed on the incident side through a φ62.51 μm GI fiberand the light receptor side of each end part of the main waveguide, anda branched waveguide is connected to a light intensity measurer througha φ200 μm HPCF-GI fiber to measure the insertion loss of the incidentlight. Also, a matching oil is used at the connecting member.

As a result of measurement, each insertion loss of incident light is:

Main waveguide: 3.8 dB

Branched waveguide: 4.7 dB.

Example 2

As shown in FIG. 8, a main waveguide is 50 μm by 50 μm and has a lengthof 10 mm, a gas cavity constituted of air has a configuration which isan isosceles triangle structure in which the sides forming a right angleare each 50 μm in length has a plane inclined at an angle of 45° in thedirection of light propagation in the main waveguide and disposed at thecenter of the main waveguide and the main waveguide which extends 10 mmin the direction at an angle of 90° in the direction of the mainwaveguide from the border of the air part. An ultraviolet ray-curablepolymer having a refractive index of 1.54 is used for a core, anultraviolet ray-curable polymer having a refractive index of 1.51 isused as a clad and ARTON FILM® (described above) is used as a top and abottom substrate. An LED having a wavelength of 850 nm is disposed onthe incident side through a φ62.5 μm GI fiber, and the main waveguideend is connected to a light intensity measurer through a φ200 μm HPCF-GIfiber, to measure the insertion loss of the incident light after theincident light is reflected. Also, a matching oil is used at theconnecting member.

As a result of measurement, the insertion loss of incident light is 1.5dB.

Example 3

Production of a Master Plate

As shown in FIG. 9A, a thick film resist is applied to a Si substrate 80by a spin coating method, then pre-baked at 80° C., subjected toexposure through a photomask, and then developed to form waveguide coreconvex portions 82 and 84 for changing the direction of lightpropagation and a concave portion 86 for a cavity in a core (core width:100 μm, cavity width: 50 cm). The substrate is post-baked at 120° C. toproduce a master plate for manufacturing an optical waveguide core and acavity in the core.

Production of a Mold

Next, after a releasing agent is applied to the master plate, aheat-curable dimethylsiloxane resin (trade name: SYLGARD184,manufactured by Dow Coning Asia Ltd.) is poured into the master plate,allowed to stand for a fixed time, then subjected to defoaming under avacuum for 10 minutes, and heated at 120° C. for 30 minutes to solidifythe resin. The solidified resin is then released to produce a mold 80Ahaving a concave portion 82A corresponding to a main waveguide, aconcave portion corresponding to a branched waveguide 84A and a convexportion 86A (thickness of the mold: 5 mm) at the place corresponding tothe cavity within the main waveguide. Moreover, cavities each having adiameter of 3 mm are opened at both ends of the main waveguide and atone end of the branched waveguide as a core filling port 90 and suctionports 92.

Then, as shown in FIG. 9C, the mold 80A is brought into close contactwith a film substrate (ARTON FILM®, described above, refractive index:1.51) 94.

Next, the core filling port 90 formed in the mold is fully filled with aultraviolet ray-curable resin (manufactured by JSR Corporation,refractive index of the cured resin: 1.54) having a viscosity of 800mPa·s to suck the resin from each suction port 92 of the end part of themain waveguide 82A and the end part of the branched waveguide 84A, withthe result that the ultraviolet ray-curable resin is filled in the mainwaveguide part, except at the gas cavity part and the branched waveguidepart.

Then, the resin in the mold is irradiated with 50 mW/cm² ultravioletlight through the aforementioned mold (dimethylsiloxane resin) for 5minutes to cure the resin and then the mold is released to produce awaveguide core having an air cavity on the ARTON FILM® (describedabove).

An ultraviolet ray-curable resin for a clad which has a viscosity of 730mPa·s and a refractive index of 1.51 is applied to the periphery of thewaveguide core provided with an air cavity on the aforementioned ARTONFILM® (described above). At this time, the clad agent does not intrudeinto the core cavity because of the viscosity specific to an uncuredpolymer. One more sheet of the above-mentioned ARTON FILM® (describedabove) is prepared and sandwiched through the clad agent.

The resin is immediately irradiated with 50 mW/cm² ultraviolet lightthrough an ARTON FILM® (described above) to cure the resin.

Finally, the mold is cut out by a dicing saw to form the end part of thewaveguide.

An optical waveguide is thus produced by the above steps.

In the aforementioned Example 3, the cavity is formed simultaneouslywhen the waveguide core is formed, and it is therefore understood thatthis process has high manufacturing efficiency.

1. An optical waveguide comprising: a waveguide core having a cavitysurrounded by the waveguide core; and a clad which encloses theperiphery of the waveguide core and has a smaller refractive index thanthe waveguide core has, wherein the optical waveguide changes adirection of a part or all of propagated light by using a part or all ofan interface between the waveguide core and the cavity as a reflectingsurface; wherein an area, in which a projected area that is obtained byprojecting the reflecting surface in the direction of the waveguide coreoverlaps with a cross-sectional plane of the waveguide core, is smallerthan a cross-sectional area of the waveguide core; and a branchedwaveguide is formed therein which divides the propagated light incidentto the waveguide core into light which reflects on the reflectingsurface and light, other than light reflected at the reflection surface,which travels in linear propagation in the waveguide core.
 2. Theoptical waveguide of claim 1, wherein the clad comprises a polymermaterial.
 3. The optical waveguide of claim 1, wherein an angle of thereflecting surface is set at an inclined angle at which the propagatedlight is totally reflected.
 4. The optical waveguide of claim 1, whereina branched waveguide core that propagates the propagated light reflectedon the reflecting surface is provided, and a sectional area of thepropagated light reflected on the reflecting surface, which isperpendicular to the direction in which the propagated light travels andis in the vicinity of the branched part, is smaller than the sectionalarea of the branched waveguide core and is contained within the branchedwaveguide.
 5. An optical waveguide according to claim 1, wherein thereflecting surface is a planar surface that is perpendicular to a planethat is parallel to (i) a direction of propagated light and (ii) adirection of reflected light.
 6. An optical waveguide comprising: awaveguide core having a cavity surrounded by the waveguide core; and aclad which encloses the periphery of the waveguide core and has asmaller refractive index than the waveguide core has, wherein theoptical waveguide changes a direction of a part or all of propagatedlight by using a part or all of an interface between the waveguide coreand the cavity as a reflecting surface; wherein an area, in which aprojected area that is obtained by projecting the reflecting surface inthe direction of the waveguide core overlaps with a cross-sectionalplane of the waveguide core, is identical to a cross-sectional area ofthe waveguide core; and the waveguide core is set so as to be largeronly at a portion where the cavity is present.
 7. The optical waveguideof claim 6, wherein the clad comprises a polymer material.
 8. Theoptical waveguide of claim 6, wherein an angle of the reflecting surfaceis set at an inclined angle at which the propagated light is totallyreflected.
 9. An optical waveguide according to claim 6, wherein thereflecting surface is a planar surface that is perpendicular to a planethat is parallel to (i) a direction of propagated light and (ii) adirection of reflected light.
 10. An optical waveguide comprising: awaveguide core having a cavity surrounded by the waveguide core; and aclad which encloses the periphery of the waveguide core and has asmaller refractive index than the waveguide core has, wherein theoptical waveguide changes a direction of a part or all of propagatedlight by using a part or all of an interface between the waveguide coreand the cavity as a reflecting surface; and wherein at least one of bothend portions on a diagonal face of the reflecting surface is positionedoutside of a line extending from an outside periphery of the waveguidecore at the upstream side in the direction in which the propagated lighttravels, and the waveguide core at the cavity location is enlarged tosurround the cavity.
 11. The optical waveguide of claim 10, wherein theclad comprises a polymer material.
 12. The optical waveguide of claim10, wherein an angle of the reflecting surface is set at an inclinedangle at which the propagated light is totally reflected.
 13. An opticalwaveguide according to claim 10, wherein the reflecting surface is aplanar surface that is perpendicular to a plane that is parallel to (i)a direction of propagated light and (ii) a direction of reflected light.